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Certification
Agilent Technologies Inc. certifies that this product met
its published specifications at the time of shipment from
the factory.
Agilent Technologies further certifies that its calibration
measurements are traceable to the United States
National Institute of Standards and Technology, NIST
(formerly the United States National Bureau of
Sta ndar ds, N BS) t o the exte nt allowed by the In sti tutes ’s
calibration facility, and to the calibration facilities of
other International Standards Organization members.
ISO 9001 Certification
Produced to ISO 9001 international quality system
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Sixth Edition
81680-90014 E0101
First Edition:
E0599: May 1999
Second Edition:
E1099: October 1999
Third Edition:
E1299: December 1999
Fourth Edition:
E0300: March 2000
Fifth Edition:
E0900: September 2000
Sixth Edition:
E0101: January 2001
Limitation of Warranty
The foregoing warranty shall not apply to defects
resulting from improper or inadequate maintenance by
Buyer, Buyer-supplied software or interfacing,
unauthorized modification or misuse, operation outside
of the environmental specifications for the product, or
improper site preparation or maintenance.
No oth er warran ty is expre ssed or implied. Agilent
Technologies specifically disclaims the implied
warranties of Merchantability and Fitness for a
Particular Purpose.
WARNINGThe WARNING sign denotes a hazard. It calls attention to a procedure,
Safety Summary
The following general safety precautions must be observed during all
phases of operation, service, and repair of this instrument. Failure to
comply with these precautions or with specific warnings elsewhere in
this manual violates safety standards of design, manufacture, and
intended use of the instrument. Agilent Technologies Inc. assumes no
liability for the customer’s failure to comply with these requirements.
Before operation, review the instrument and manual, including the
red safety page, for safety markings and instructions. You must follow
these to ensure safe operation and to maintain the instrument in safe
condition.
practice or the like, which, if not correctly performed or adhered to,
could result in injury or loss of life. Do not proceed beyond a
WAR N I NG sign u ntil th e indica t ed conditions ar e fully u nd ersto od a nd
met.
Safety Symbols
The apparatus will be marked with this symbol when it is necessary
for the user to refer to the instruction manual in order to protect the
apparatus against damage.
Hazardous laser radiation.
Initial Inspection
Inspect the shipping container for damage. If there is damage to the
container or cushioning, keep them until you have checked the
contents of the shipment for completeness and verified the instrument
both mechanically and electrically.
The Performance Tests give procedures for checking the operation of
the instrument. If the contents are incomplete, mechanical damage or
defect is apparent, or if an instrument does not pass the operator’s
checks, notify the nearest Agilent Technologies Sales/Service Office.
WARNINGTo avoid hazardous electrical shock, do not perform electrical tests
when there are signs of shipping damage to any portion of the outer
enclosure (covers, panels, etc.).
WARNINGYou MUST return instruments with malfunctioning laser modules to
an Agilent Technologies Sales/Service Center for repair and
calibration.
Line Power Requirements
The Agilent 81480A, Agilent 81680A, Agilent 81640A, Agilent 81682A,
Agilent 81642A, & Agilent 81689A Tunable Laser Modules operate
when installed in the Agilent 8164A Lightwave Measurement System.
The Agilent 81689A also operates when installed in the Agilent 8163A
Lightwave Multimeter or Agilent 8166A Lightwave Multichannel
System.
Operating Environment
The safety information in the Agilent 8163A Lightwave Multimeter,
Agilent 8164A Lightwave Measurement System, & Agilent 8166A
Lightwave Multichannel System User’s Guide summarizes the
operating ranges for the Agilent 81480A, Agilent 81680A,
Agilent 81640A, Agilent 81682A, Agilent 81642A, & Agilent 81689A
Tunable Laser Modules. In order for these modules to meet
specifications, the operating environment must be within the limits
specified for your mainframe.
Input/Output Signals
CAUTIONThere are two BNC connectors on the front panel of the
Agilent 81480A, Agilent 81680A, Agilent 81640A, Agilent 81682A, and
Agilent 81642A; a BNC input connector and a BNC output connector.
There is one BNC connector on the front panel of the Agilent 81689A a BNC input connector.
An absolute maximum of ±6 V can be applied as an external voltage to
any BNC connector.
Storage and Shipment
This module can be stored or shipped at temperatures between
−40°C and +70°C. Protect the module from temperature extremes that
may cause condensation within it.
Laser Class according to
IEC 60825-1 (1998)- International
Max. permissible CW output
power - IEC**
Laser Class according to
FDA 21 CFR 1040.10 (1995) - USA
Max. permissible CW output
power - FDA**
* Max. CW output power is defined as the highest possible optical power that the laser source can produce at its output connector.
** Max. permissible CW output power is the highest optical power that is permitted within the appropriate laser class.
A sheet of laser safety warning labels are included with the
instrument. You MUST stick the labels in the local language onto the
outside of the instrument, in a position where they are clearly visible
to anyone using the instrument.
Top Vi e w
See page 6See page 6
Figure 3Position of Safety Labels on Backloadable Tunable Laser Modules
These labels are applied in these positions to every Agilent 81480A,
Agilent 81680A, Agilent 81640A, Agilent 81682A, and Agilent 81642A
Tunable Laser Module before shipment.
See page 6
Figure 4Position of Safety Labels on Agilent 81689A Tunable Laser Module
These labels are applied in these positions to every Agilent 81689A
Tunable Laser Module before shipment.
Safety Symbols3
Initial Inspection3
Line Power Requirements4
Operating Environment4
Input/Output Signals4
Storage and Shipment4
Initial Safety Information for Tunable Laser Modules5
Laser Safety Labels 6
Preserving Connectors179
Cleaning Instrument Housings179
Which Cleaning Procedure should I use ?180
How to clean connectors180
How to clean connector adapters181
How to clean connector interfaces182
What is a Tunable Laser ?Getting Started with Tunable Laser Sources
What is a Tunable Laser ?
A Tunable Laser is a laser source for which the wavelength can be
varied through a specified range. The Agilent Technologies range of
Tunable Laser modules also allow you to set the output power, and to
choose between continuous wave or modulated power.
What is a Tunable Laser ?Getting Started with Tunable Laser Sources
The Agilent 81480A and 81680A/82A/40A/42A Tunable Laser
modules are back-loadable modules. To fit these modules into the
Agile nt 8164A mainframe see “How to Fit and Remove Modules” in th e
Agilent 8163A Lightwave Multimeter, Agilent 8164A, Lightwave
Measurement System, & Agilent 8166A Lightwave Multichannel
SystemUser’s Guide.
The Agilent 81480A and 81680A/82A/40A/42A Tunable Laser
modules have a built-in wavelength control loop to ensure high
wavelength accuracy. As these modules are all mode-hop free tunable
with continuous output power, they qualify for the test of the most
critical dense-Wavelength Division Multiplexer (dWDM) components.
The Agilent 81480A and Agilent 81640A/80A Tunable Laser modules
are equipped with two optical outputs:
• Output 1, the Low SSE output, delivers a signal with ultra-low
source spontaneous emission (SSE). It enables accurate crosstalk
measurement of DWDM components with many channels at narrow
spacing. You can characterize steep notch filt ers such as Fiber
Bragg Gratings by using this output and a power sensor module.
• Output 2, the High Power output, delivers a signal with high optical
power. You can adjust the signal by more than 60 dB by using the in-
built optical attenuator.
The Agilent 81682A/42A Tunable Laser module delivers a signal with
high optical power. If you choose O ption 0 03 , you can adjust the signal
by more than 60 dB by using the in-built optical attenuator.
Getting Started with Tunable Laser SourcesWhat is a Tunable Laser ?
Agilent 81689A Tunable Laser Module
Agilent 81689A with
Straight Contact Connector
Figure 10Agilent 81689A Tunable Laser Module
The Agilent 81689A Tunable Laser module is a front-loadable module.
To insert this module into the Agilent 8163A Lightwave Multimeter,
Agilent 8164A Lightwave Measurement System or Agilent 8166A
Lightwave Multichannel System see “How to Fit and Remove Modu les”
in the Agilent 8163A Lightwave Multimeter, Agilent 8164A Lightwave
Measurement System, & Agilent 8166A Lightwave Multichannel
System User’s Guide.
You can use the Agilent 81689A Tunable Laser module to set up a
realistic multi-channel test-bed for DWDM transmission systems. Its
continuous, mode-hop free tuning makes it quick and easy to set even
the most complex configurations to the target wavelengths and power
levels.
The Agilent 8163A Lightwave Multimeter, a Power Sensor module,and
a Agilent 81689A Tunable Laser module together represent a smart
loss-test set with selectable wavelength.
Optical OutputGetting Started with Tunable Laser Sources
Optical Output
Polarization Maintaining Fiber
If you have an instrument with a polarization maintaining fiber (PMF),
the PMF is aligned to maintain the state of polarization.
The fiber is of Panda type, with TE mode in the slow axis in line with
the connector key. A well defined state of polarization ensures
constant measurement conditions.
The Agilent 81480A and 81680A/40A/82A/42A Tunable Laser
modules are equipped with PMF outputs as standard.
For the Agilent 81689A Tunable Laser module, PMF output is available
as an option.
Stress Rods
Figure 11PMF Output Connector
Angled and Straight Contact Connectors
Angled contact connectors help you to control return lo ss. With angled
fiber endfaces, reflected light tends to reflect into the cladding,
reducing the amount of light that reflects back to the source.
E
Connector Key
Fiber Cladding
H
Fiber Core
(8-µm Diameter)
Slow Axis (Polarization Axis)
Not to Scale
The Agilent 81480 and 81680A/40A/82A/42A/89A Tunable Laser
modules can have the following connector interface options:
Getting Started with Tunable Laser SourcesOptical Output
Two additional connector interface options are available for the
Agilent 81689A Tunable Laser module:
• Option 021, Standard single-mode fiber straight contact connectors,
or
• Option 022, Standard single-mode fiber angled contact connectors.
CAUTIONIf the contact connector on your instrument is angled, you can only
use cables with angled connectors with the instrument.
Angled Contact
Connector Symbol
Figure 12Angled and Straight Contact Connector Symbols
Figure 12 shows the symbols that tell you whether the contact
connector of your Tunable Laser module is angled or straight. The
angled contact connector symbol is colored green.
Figure 7 and Figure 13 show the front panel of the Agilent 81682A
Tunable Laser module with straight and angled contact connectors
respectively.
You should connect straight contact fiber end connectors with neutral
sleeves to straight contact connectors and connect angled contact fiber
end connectors with green sleeves to angled contact connectors.
NOTEYou cannot connect angled non-contact fiber end connectors with
The Agilent 8164A Lightwave Measurement System supports the
Agilent 81480A and 81680A/40A/82A/42A/89A Tunable Laser
modules. In addition, the Agilent 8163A Lightwave Multimeter
supports the Agilent 81689A Tunable Laser module.
Tunable Laser Modules
Model No.Description
Agilent 81480ATunable Laser for the Test of Critical dense-WDM Components
Agilent 81680ATunable Laser for the Test of Critical dense-WDM Components
Agilent 81640ATunable Laser for the Test of Critical Components in both
dense-WDM Bands, the C and L bands
Agilent 81682ATunable Laser for the Test of Optical Amplifiers and Passive
Components
Agilent 81642ATunable Laser for the Test of Optical Amplifiers and Passive
Components in both dense-WDM Bands.
Agilent 81689ATunable Laser for Multi-Channel Test Applications
Filler Module
Filler Module
Model No.Description
Agilent 81645AFiller Module
The Agilent 81645A Filler Module is required to operate the
Agile nt 8164A mainframe if it is used without a back-loadable Tunable
Laser module. It can be used to:
• prevent dust pollution and
• optimize cooling by guiding the air flow.
See the "Installation and Maintenance" chapter of the Agilent 81480A,
Agilent 81680A, Agilent 81682A, Agilent 81640A, & Agilent 81689A
Tunable Laser Modules User’s Guide for more details on installing the
Agilent 81645A Filler Module.
Two additional connector interface options are available for the
Agilent 81689A Tunable Laser module:
• Option 021, Standard single-mode fiber straight contact connectors,
or
• Option 022, Standard single-mode fiber angled contact connectors.
Options 071, 021: Straight Contact
Connectors
If you want to use straight connectors (such as FC/PC, Diamond HMS10, DIN, Biconic, SC, ST or D4) to connect to the instrument, you must
do the following:
This section defines terms that are used both in this chapter and
“Performance Tests” on page 57.
Generally, all specifications apply for the given environmental
conditions and after warmup time.
Measurement principles are indicated. Alternative measurement
principles of equal value are also acceptable.
Absolute Wavelength Accuracy
The maximum difference between the actual wavelength and the
displayed wavelength of the TLS. Wavelength is defined as wavelength
in vacuum.
Conditions: constant power level, temperature within operating
temperature range, coherence control off, measured at high power
output.
Validity: within given time span after wavelength zeroing, at a given
maximum temperature difference between calibration and
measurement.
Measurement with wavelength meter. Averaging time given by
wavelength meter, ≥1 s.
NOTEThe abso lute wavelength accuracy of Output 1, the Lo w SSE Ou tput, of
the Agilent 81680A/40A Tunable Laser modules is the same as the
absolute wavelength accuracy of Output 2, the High Power Output
(guaranteed by design).
Effective Linewidth
The time-averaged 3-dB width of the optical spectrum, expressed in
Hertz.
Conditions: temperature within operating temperature range,
coherence control on, power set to specified value.
Measurement with heterodyning technique: the output of the laser
under test is mixed with another laser of the same type on a wide
bandwidth photodetector. The electrical noise spectrum of the
photodetector current is measured with an Agilent Lightwave Signal
Analyzer, and the linewidth is calculated from the heterodyne
spectrum (Lightwave signal analyzer settings: resolution bandwidth
1 MHz; video bandwidth 10 kHz; sweep time 20 ms; single scan).
Linewidth
The 3-dB width of the optical spectrum, expressed in Hertz.
Conditions: temperature within operating temperature range,
coherence control off, power set to maximum flat power (maximum
attainable power within given wavelength range).
Measurement with self-heterodyning technique: the output of the
laser under test is sent through a Mach-Zehnder interferometer in
which the length difference of the two arms is longer than the
coherence length of the laser. The electrical noise spectrum of the
photodetector current is measured with an Agilent Lightwave Signal
Analyzer, and the linewidth is calculated from the heterodyne
spectrum (Lightwave signal analyzer settings: resolution bandwidth 1
MHz; video bandwidth 10 kHz; sweep time 20 ms; single scan).
Minimum Output Power
The minimum output power for which the specifications apply.
Mode-Hop Free Tuning Range
The tuning range for which no abrupt wavelength change occurs
during fine wavelength stepping. Abrupt change is defined as change
of more than 25 pm.
Conditions: within specified wavelength range, at specified
temperature range and output power. Tuning from outside into the
mode-hop free tuning range is not allowed.
Modulation Extinction Ratio
The ratio of total power in on-state to total power in off-state,
expressed in dB.
Conditions: Internal or external modulation, tunable laser at highest
power setting.
Measurement with optical spectrum analyzer. Tunable laser switched
on and off.
Modulation Frequency Range
The range of frequencies for which the modulation index is above − 3
dB of the highest modulation index. In this context, modulation index
is defined as the AC power amplitude (peak-to-peak) divided by the
average power.
Output Power
The achievable output power for the specified TLS tuning range.
Conditions: temperature within operating temperature range.
Measurement with power meter at the end of a single-mode fiber
patchcord.
Output Isolation
The insertion loss of the built-in isolator in the backward direction.
Measurement: Cannot be measured from the outside. This
characteristic is based on known isolator characteristics.
Peak Power
The highest optical power within specified wavelength range.
Polarization Extinction Ratio
The ratio of optical power in the slow axis of the polarizationmaintaining fiber to optical power in the fast axis within a specified
wavelength range.
Conditions: only applicable for TLS with polarization maintaining
fiber with the TE mode in slow axis and oriented in line with
connector key, at constant power level.
Measurement with a polarization analyzer at the end of a polarizationmaintaining patchcord, by sweeping the wavelength, thereby creating
circular traces on the Poincaré sphere, then calculating the
polarization extinction ratio from the circle diameters.
When changing the wavelength and modulation frequency, and
measuring the differences between actual and displayed power levels
(in dB), the power flatness is ± half the span between the maximum
and the minimum value of all differences.
Conditions: uninterrupted line voltage, constant power setting,
temperature within ±2 K, external modulation ON.
Measurement with optical power meter.
Power Flatness Versus Wavelength
When changing the wavelength at constant power setting and
recording the differences between actual and displayed power levels,
the power flatness is ± half the span (in dB) between the maximum
and the minimum of the measured power levels.
Conditions: uninterrupted TLS output power, constant power setting,
temperature within ±1K.
Measurement with optical power meter.
Power Linearity
When changing the power level and measuring the differences (in dB)
between actual and displayed power levels, the power linearity is ±
half the span (in dB) between the maximum and the minimum value of
all differences.
Conditions: power levels from within specified output power range,
uninterrupted TLS output power, at fixed wavelength settings and
stable temperature.
Measurement with optical power meter.
Power Repeatability
The random uncertainty in reproducing the power level after changing
and re-setting the power level. The power repeatability is ± half the
span (in dB) between the highest and lowest actual power.
Conditions: uninterrupted TLS output power, constant wavelength,
temperature within ±1 K, short time span.
Measurement with optical power meter.
NOTEThe long-term power repeatability can be obtained by taken the power
The change of the power level during given time span, expressed as ±
half the span (in dB) between the highest and lowest actual power.
Conditions: uninterrupted TLS output power, constant wavelength
and power level settings, temperature within ±1 K, time span as
specified.
Measurement with optical power meter.
Relative Intensity Noise (RIN)
The square of the (spectrally resolved) RMS optical power amplitude
divided by the measurement bandwidth and the square of the average
optical power, expressed in dB/Hz.
Conditions: at specified output power, coherence control off,
temperature within operating temperature range, frequency range 0.1
to 6 GHz.
Measurement with Agilent Lightwave Signal Analyzer.
Relative Wavelength Accuracy
When randomly changing the wavelength and measuring the
differences between the actual and displayed wavelengths, the relative
wavelength accuracy is ± half the span between the maximum and the
minimum value of all differences.
Conditions: uninterrupted TLS output power, constant power level,
temperature within operating temperature range, observation time 10
minutes maximum (constant temperature), coherence control off,
measured at high power output.
Measurement with wavelength meter. Averaging time given by
wavelength meter, ≥1 s.
NOTEThe relative wavelength accuracy of Output 1, the Low SSE Output, of
the Agilent 81640A/80A Tunable Laser modules is the same as the
relative wavelength accuracy of Output 2, the High Power Output
(guaranteed by design).
Return Loss
The ratio of optical power incident to the TLS outpu t port, at the TLS's
own wavelength, to the power reflected from the TLS output port.
The ratio of average signal power to the optical power of the highest
sidemode within a distance from 0.1 to 6 GHz to the signal's optical
frequency, expressed in dB.
Conditions: at a specified output power and wavelength range,
temperature within operating temperature range, coherence control
off.
Measurement with the Agilent Lightwave Signal Analyzer, by
analyzing the heterodyning between the main signal and the highest
sidemode.
Signal-to-Source Spontaneous Emission
(SSE) Ratio
The ratio of signal power to maximum spontaneous e mission power in
1 nanometer bandwidth within a ±3 nm window around the signal
wavelength, where ±1 nm around the signal wavelength are excluded,
at the specified output power, expressed in dB/nm.
Conditions: output power set to specified values, at temperatures
within operating temperature range, coherence control off.
Measurement with optical spectrum analyzer (OSA) at 0.5 nm
resolution bandwidth (to address the possibility of higher SSE within
a narrower bandwidth), then extrapolated to 1 nm bandwidth. On
low-SSE output (if applicable), with fiber Bragg grating inserted
between the TLS and the OSA in order to suppress the signal, thereby
enhancing the dynamic range of the OSA.
NOTEThe specified signal-to-SSE ratio is also applicable to output powers
higher than the specified values.
Signal-to-Total-Source Spontaneous
Emission
The ratio of signal power to total spontaneous emission power, at the
specified achievable output power, expressed in dB.
Conditions: output power set to specified values, at temperatures
within operating temperature range, coherence control off.
Measurement with optical spectrum analyzer, by integrating the
source spontaneous emission and excluding the remnant signal. On
low-SSE output (if applicable), with fiber Bragg grating inserted
between the TLS and the OSA in order to suppress the signal, thereby
enhancing the dynamic range of the OSA.
NOTEThe specified signal-to-total-SSE ratio is also applicable to output
powers higher than the specified values.
Wavelength Range
The range of wavelengths for which the specifications apply.
Wavelength Repeatability
The random uncertainty in reproducing a wavelength after detuning
and re-setting the wavelength. The wavelength repeatability is ± half
the span between the maximum and the minimum value of all actual
values of this wavelengths.
Conditions: uninterrupted TLS output power, constant power level,
temperature within operating temperature range, coherence control
off, short time span.
Measurement wit h w a veleng th m eter a t high power o u t put. Ave r a ging
time given by wavelength meter, ≥1 s.
NOTEThe wavelength repeatability of Output 1, the Low SSE Output, of the
Agile nt 81680A/40A Tunable Laser modules is the same as th e relative
wavelength accuracy of Output 2, the High Power Output (guaranteed
by design).
NOTEThe long-term wavelength repeatability can be obtained by taken the
wavelength repeatability and wavelength stability into account.
Wavelength Resolution
The smallest possible displayed wavelength increment/decrement.
Wavelength Stability
The change of wavelength during given time span, expressed as ± half
the span between the maximum and the minimum of all actual
wavelengths.
Conditions: uninterrupted TLS output power, constant wavelength
and power level settings, coherence control off, temperature within ±1
K, time span as specified.
Measurement with wavelength meter. Averaging time given by
wavelength meter, ≥1 s.
Coherence Control (Agilent 81480A, Agilent
81680A/40A/82A/42A)
For measurements on components with 2-meter long patchcords and connectors
with 14 dB return loss, the effective linewidth results in a typical power stability of <
the test setup.
±0.025 dB over 1 minute by drastically reducing interference effects in
The equipment required for the Performance Test is listed in
Table Table 4. Any equipment which satisfies the critical
specifications of the equipment given in Table Table 4, may be
substituted for the recommended models.
Table 4Equipment Required
InstrumentDescription of Instrument/Accessory#021, #071#022, #072
Results of the performance test may be tabulated in the Test Record
provided at the end of the test procedures. It is recomm ended that you
fill out the Test Record and refer to it while doing the test. Since the
test limits and setup information are printed on the Test Record for
easy reference, the record can also be used as an abbreviated test
procedure (if you are already familiar with the test procedures). The
Test Record can also be used as a permanent record and may be
reproduced without written permission from Agilent Technologies.
Test Failure
Always ensure that you use the correct cables and adapters, and that
all connectors are undamaged and extremely clean.
If the Agilent 81480A or Agilent 81680A/40A/82A/42A/89A Tunable
Laser module fails any performance test, return the instrument to the
nearest Agilent Technologies Sales/Service Office for repair.
Instrument Specification
Specifications are the performance characteristics of the instrument
which are certified. These specifications, listed in “Specifications” on page 39, are the performance standards or limits against which the
Agilent 81480A and Agilent 81680A/40A/82A/42A/89A Tunable Laser
modules can be tested.
The specifications also list some supplemental characteristics of the
Agilent 81480A and Agilent 81680A/40A/82A/42A/89A Tunable Laser
modules. Supplemental characteristics should be considered as
additional information.
Any changes in the specifications due to manufacturing changes,
design, or traceability to the National Institute of Standards and
Technology (NIST), will be covered in a manual change su pplement, or
revised manual. Such specifications supersede any that were
previously published.
NOTE• Make sure that all fiber connectors are clean.
• Turn the instruments on, enable the laser and allow the
instruments to warm up.
• Ensure that the Device Under Test (DUT) and all the test
equipment is held within the environmental specifications given
in “Specifications” on page 39
General Test Setup
Insert your Tunable Laser module into the Agilent 8164A Lightwave
Measurement System. Insert an Agilent 81480A, Agilent 81680A,
Agilent 81640A, Agilent 81682A, or Agilent 81642A Tunable Laser
module from the rear. Insert an Agilent 81689A Tunable Laser module
from the front into slot 1 of the Agilent 8164A Lightw ave Measurement
System.
Wavelength Tests
NOTEWhen performing wavelength tests, zero the Tunable Laser first.
Move to Channel 0, press [Menu], select <λ Zeroing>.
Zeroing takes approximately 2 minutes.
Connect the Tunable Laser module to the Wavelength Meter as shown
in Figure 17.
If you use the Agilent 81480A, Agilent 81680A or Agilent 81640A
Tunable Laser module, connect the Output 2, the high power output.
Agilent 8164A Lightwave
Measurement System
Tunable Laser
For #021, #071: use 81000AI and 81101PC
For #022, #072: use 81000SI and 81113PC
Calibration of the Agilent 81001FF Attenuation Filter
NOTEWhen an HP 81524A Optical Head is used in conjunction with a
Agile nt 81001FF Attenuation Filter, it is absolutely necessary that you
calibrate the Agilent 81001FF Attenuation Filter before starting the
power tests in the following measurement setups; it is not sufficient to
use calibration factors that are derived from an earlier setup.
1 Make sure all instruments have warmed up.
Agilent 8164A Lightwave
Measurement System
Tunab le L ase r
For #021, #071: use 81000FI and 81113PC
For #022, #072: use 81000SI and 81113SC
Figure 18Calibration of the Agilent 81001FF Attenuation Filter, Reference Setup
2 Set the power meter installed in the HP 8153A to the following
values:
aSet range to 0 dBm; press Up or Down as required.
b Set T, the averaging time, to 500 ms.
cAgilent 81680A, 40A, 82A, 42A, & 89A:
Set λ, the wavelength, to 1550 nm.
Agilent 81480A:
Set λ, the wavelength, to 1450 nm.
Agilent 81000SA
Slanted
Connector
HP 81524A
Optical Head
HP 8153A Lightwave Multimeter
HP 81533B
d Select dBm as the power units.
3 Move to the Tunable Laser channel of the Agilent 8164A.
Agilent 81680A, 40A, 82A, 42A, & 89A:
Set λ, the wavelength, to 1550 nm, and [P], the power, to 0 dBm..
For Agilent 81480A:
Set λ, the wavelength, to 1450 nm, and [P], the power, to 0 dBm.
4 Press the key beside the laser output to switch the laser on.
Follow the steps below to measure the power linearity (while using
attenuation) of any one of the following:
• Output 2, the High Power output, of the Agilent 81480A
• Output 2, the High Power output, of the Agilent 81680A
• Output 2, the High Power output, of the Agilent 81640A
• Agilent 81682A #003
• Agilent 81642A #003
1 Set up the equipment as shown in Figure 21.
2 Move to the Tunable Laser channel of the Agilent 8164A Lightwave
Measurement System and press [Menu].
3 Set the menu parameters to the values shown in Table Table 5.
For Agilent 81480A, Agilent 81680A, Agilent 81640A,
Agilent 81642A#003 Agilent 81682A#003:
Set < Power Mode> to <ManualAtt>.
4 Set th e wavelength and power for each Tunable Laser modu le to the
values given in Table Table 13.
Table 13Wavelength and Power Settings for High Power Linearity Tests with
Attenuation
ModuleWavelength [λ]Power [P]Attenuation [Atten]
Agilent 81480A - Output 21430.000 nm+0.000 dBm0.000 dB
Agilent 81680A - Output 21540.000 nm+0.000 dBm0.000 dB
Agilent 81640A - Output 21560.000 nm+0.000 dBm0.000 dB
Agilent 81682A #0031540.000 nm+0.000 dBm0.000 dB
Agilent 81642A #0031580.000 nm+0.000 dBm0.000 dB
NOTEIf you use the Agilent 81480A Output 2, Agilent 81680A Output 2, or
Agilent 81640A Output 2 with attenuation, use the table “Power
Linearity Output 2, High Power by attenuator” on page 121 or “Power
Linearity Output 2, High Power by Attenuator” on page 135
respectively.
If you use the Agilent 81682A #003 with attenuation, use the table
“Power Linearity 81682A #003 by Attenuator” on page 149.
If you use the Agilent 81642A #003 with attenuation, use the table
“Power Linearity 81642A #003 by Attenuator” on page 161.
5 Perform the steps 5 to 16 of the “Power Linearity - Low Power Test”
Follow this procedure to test modules with Low SSE high power
outputs:
• Agilent 81480A, Output 1, Low SSE
• Agilent 81680A, Output 1, Low SSE
• Agilent 81640A, Output 1, Low SSE
The previous setup is limited by the dynamic range of the Optical
Spectrum Analyzer. An improvement can be done by reducing the
power of the spectral line of the Tunable Laser module by a filter, a
Fiber Bragg Grating. However, by this approach, the measurement is
limited to a single wavelength (that of the peak attenuation of the
Fiber Bragg Grating):
The Fiber Bragg Grating has a straight connector on one end and a
slanted connector on the other. Depending on the output connector
option of your Tunable Laser module, the Device Under Test (DUT),
the Fiber Bragg Grating should be connected with:
• a straight connector, if you use option #021 or #071, or
• the slanted connector, if you use option #022 or #072.
NOTEBecause the Tunable Laser channel displays the wavelength in air and
the Optical Spectrum Analyzer displays the wavelength in a vacuum
there is a mismatch between the values displayed by the two
instruments.
A good approximation in this wavelength range is:
= λ
λ
OSA
Use λ
accuracy of the Tunable Laser modules is better than the OSA.
The accuracy of the offset value in this equ ation d oes not influence the
measurement accuracy of spectral and total SSE measurements.
as primary reference because the specified wavelength
With a sampling step of 1 nm on the OSA, check all 201 power
levels within the recorded spectrum, sta rting at OSA_l_center –
15 nm and finishing at OSA_l_center + 15 nm.
NOTENote the “partial noise power level” values in a table in [pW], where
1 pW = 10
Example:
Table 20Signal to Total SSE Tests - Low SSE Outputs
Wavelength,
Relative to OSA_λ_centerPartial Noise Power levels
−15 nm pW
−14 nm pW
−13nm pW
…. pW
…. pW
−2nm pW
−1nm pW
−12
W.
±0nm (= OSA_λ_center) pW
+1 nm pW
+2 nm pW
…. pW
…. pW
+13 nm pW
+14 nm pW
+ 15 nm pW
Sum of all partial noise power levels pW
eDetermine total noise power by adding up all 31 partial noise
power levels:
OSA_noise = Sum of all partial noise power levels
OSA_noise = _________ pW
fNote the OSA_noise value in the test record.
3 Connect the Tunable Laser (DUT) to the Optical Spectr um Analyzer
as shown in Figure 25. Connect one end of the Fiber Bragg Grating
to Output 1,the Low SSE output of the TLS and the other to the
Optical Spectrum Analyzer.
4 Set the TLS menu parameters to the values shown in Table Table 5.